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Towards optimized surface $\delta$-profiles of nitrogen-vacancy centers activated by helium irradiation in diamond

机译:接近优化的表面$ \ delta $ -profiles的氮空位中心   金刚石中的氦辐射激活

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摘要

The negatively-charged nitrogen-vacancy (NV) center in diamond has been shownrecently as an excellent sensor for external spins. Nevertheless, their optimumengineering in the near-surface region still requires quantitative knowledge inregard to their activation by vacancy capture during thermal annealing. To thisaim, we report on the depth profiles of near-surface helium-induced NV centers(and related helium defects) by step-etching with nanometer resolution. Thisprovides insights into the efficiency of vacancy diffusion and recombinationpaths concurrent to the formation of NV centers. It was found that the range ofefficient formation of NV centers is limited only to approximately $10$ to$15\,$nm (radius) around the initial ion track of irradiating helium atoms.Using this information we demonstrate the fabrication of nanometric-thin($\delta$) profiles of NV centers for sensing external spins at the diamondsurface based on a three-step approach, which comprises (i) nitrogen-dopedepitaxial CVD diamond overgrowth, (ii) activation of NV centers by low-energyhelium irradiation and thermal annealing, and (iii) controlled layer thinningby low-damage plasma etching. Spin coherence times (Hahn echo) ranging up to$50\,$ $\mu$s are demonstrated at depths of less than $5\,$nm in material with$1.1\,\%$ of $^{13}$C (depth estimated by spin relaxation (T$_1$)measurements). At the end, the limits of the helium irradiation technique athigh ion fluences are also experimentally investigated.
机译:金刚石中带负电荷的氮空位(NV)中心最近被证明是用于外部自旋的出色传感器。尽管如此,它们在近表面区域的最佳工程设计仍需要定量知识,而不论它们在热退火过程中是通过空位捕获来激活的。为此,我们以纳米分辨率逐步蚀刻报告了近表面氦诱导的NV中心(及相关的氦缺陷)的深度分布。这为洞察扩散和重组路径与NV中心形成同时发生的效率提供了见解。研究发现,NV中心有效形成的范围仅限于辐照氦原子的初始离子轨道周围约$ 10 $至$ 15 \,$ nm(半径)。 δ)基于三步法的NV中心轮廓,用于感测钻石表面的外部自旋,包括(i)氮掺杂外延CVD金刚石的过度生长,(ii)通过低能氦辐照和热退火激活NV中心;以及(iii)通过低损伤等离子体刻蚀来控制层变薄。在材料深度小于$ 5 \,$ nm的情况下,自旋相干时间(Hahn回声)高达$ 50 \,$$ \ mu $ s,其中$ ^ {13} $ C($ 1.1通过自旋弛豫(T $ _1 $)测量值估算)。最后,还通过实验研究了高离子通量下氦气辐照技术的局限性。

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